Abstract

We report on the generation of a multi-octave, phase-stable continuum from the output of a Yb:YAG regenerative amplifier delivering 1-ps pulses with randomly varying carrier-envelope phase (CEP). The intrinsically CEP-stable spectral continuum spans from 450 nm to beyond 2500 nm, covering a spectral range of about 0.6 PHz. The generated coherent broadband light carries an energy of 4 μJ, which can be scaled to higher values if required. The system has been designed and is ideally suited for seeding broadband parametric amplifiers and multichannel synthesizers pumped by picosecond Yb:YAG amplifiers, obviating the need for active timing synchronization required in previous approaches. The presented concept paves the way to cost-effective, reliable all-Yb:YAG single-cycle sources with terawatt peak-power and tens-of-Watts average power.

© 2016 Optical Society of America

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2016 (5)

2015 (9)

M. Puppin, Y. Deng, O. Prochnow, J. Ahrens, T. Binhammer, U. Morgner, M. Krenz, M. Wolf, and R. Ernstorfer, “500 kHz OPCPA delivering tunable sub-20 fs pulses with 15 W average power based on an all-ytterbium laser,” Opt. Express 23, 1491–1497 (2015).
[Crossref] [PubMed]

S. Prinz, M. Haefner, C. Y. Teisset, R. Bessing, K. Michel, Y. Lee, X. T. Geng, S. Kim, D. E. Kim, T. Metzger, and M. Schultze, “CEP-stable, sub-6 fs, 300-kHz OPCPA system with more than 15 W of average power,” Opt. Express 23, 1388–1394 (2015).
[Crossref] [PubMed]

Y. Shamir, J. Rothhardt, S. Hädrich, S. Demmler, M. Tschernajew, J. Limpert, and A. Tünnermann, “High-average-power 2 μm few-cycle optical parametric chirped pulse amplifier at 100 kHz repetition rate,” Opt. Lett. 40, 5546–5549 (2015).
[Crossref] [PubMed]

O. Pronin, M. Seidel, F. Lücking, J. Brons, E. Fedulova, M. Trubetskov, V. Pervak, A. Apolonski, T. Udem, and F. Krausz, “High-power multi-megahertz source of waveform-stabilized few-cycle light,” Nat. Commun. 6, 1–6 (2015).
[Crossref]

L. E. Zapata, H. Lin, A.-L. Calendron, H. Cankaya, M. Hemmer, F. Reichert, W. R. Huang, E. Granados, K.-H. Hong, and F. X. Kärtner, “Cryogenic Yb:YAG composite-thin-disk for high energy and average power amplifiers,” Opt. Lett. 40, 2610–2613 (2015).
[Crossref] [PubMed]

L. Lötscher and L. Vámos, “Long-term stability of nonlinear pulse compression using solid-core large-mode-area fibers,” J. Lasers Opt. Photonics 02, 1–5 (2015).
[Crossref]

J. Galinis, G. Tamošauskas, I. GraŽulevičiute, E. Keblyte, V. Jukna, and A. Dubietis, “Filamentation and supercontinuum generation in solid-state dielectric media with picosecond laser pulses,” Phys. Rev. A - At. Mol. Opt. Phys. 92, 1–5 (2015).
[Crossref]

A.-L. Calendron, H. Çankaya, G. Cirmi, and F. X. Kärtner, “White-light generation with sub-ps pulses,” Opt. Express 23, 13866–13879 (2015).
[Crossref] [PubMed]

O. D. Mucke, S. Fang, G. Cirmi, G. M. Rossi, S.-H. Chia, H. Ye, Y. Yang, R. Mainz, C. Manzoni, P. Farinello, G. Cerullo, and F. X. Kartner, “Toward waveform nonlinear optics using multimillijoule sub-cycle waveform synthesizers,” IEEE J. Sel. Top. Quantum Electron. 21, 1–12 (2015).
[Crossref]

2014 (4)

2012 (9)

C. Homann, M. Bradler, M. Förster, P. Hommelhoff, and E. Riedle, “Carrier-envelope phase stable sub-two-cycle pulses tunable around 1.8 μm at 100 kHz,” Opt. Lett. 37, 1673–1675 (2012).
[Crossref] [PubMed]

S. Hädrich, J. Rothhardt, M. Krebs, S. Demmler, J. Limpert, and A. Tünnermann, “Improving carrier-envelope phase stability in optical parametric chirped-pulse amplifiers by control of timing jitter,” Opt. Lett. 37, 4910–4912 (2012).
[Crossref] [PubMed]

J. Rothhardt, S. Demmler, S. Hädrich, J. Limpert, and A. Tünnermann, “Octave-spanning OPCPA system delivering CEP-stable few-cycle pulses and 22 W of average power at 1 MHz repetition rate,” Opt. Express 20, 10870–10878 (2012).
[Crossref] [PubMed]

H. Fattahi, C. Y. Teisset, O. Pronin, A. Sugita, R. Graf, V. Pervak, X. Gu, T. Metzger, Z. Major, F. Krausz, and A. Apolonski, “Pump-seed synchronization for MHz repetition rate, high-power optical parametric chirped pulse amplification,” Opt. Express 20, 9833–9840 (2012).
[Crossref] [PubMed]

A. Schwarz, M. Ueffing, Y. Deng, X. Gu, H. Fattahi, T. Metzger, M. Ossiander, F. Krausz, and R. Kienberger, “Active stabilization for optically synchronized optical parametric chirped pulse amplification,” Opt. Express 20, 5557–5565 (2012).
[Crossref] [PubMed]

T. Popmintchev, M.-C. Chen, D. Popmintchev, P. Arpin, S. Brown, S. Alisauskas, G. Andriukaitis, T. Balciunas, O. D. Mücke, A. Pugzlys, A. Baltuska, B. Shim, S. E. Schrauth, A. Gaeta, C. Hernández-García, L. Plaja, A. Becker, A. Jaron-Becker, M. M. Murnane, and H. C. Kapteyn, “Bright coherent ultrahigh harmonics in the keV x-ray regime from mid-infrared femtosecond lasers,” Science 336, 1287–1291 (2012).
[Crossref] [PubMed]

M. T. Hassan, A. Wirth, I. Grguraš, A. Moulet, T. T. Luu, J. Gagnon, V. Pervak, and E. Goulielmakis, “Invited article: attosecond photonics: synthesis and control of light transients,” Rev. Sci. Instrum. 83, 1113011 (2012).
[Crossref]

Y. Deng, A. Schwarz, H. Fattahi, M. Ueffing, X. Gu, M. Ossiander, T. Metzger, V. Pervak, H. Ishizuki, T. Taira, T. Kobayashi, G. Marcus, F. Krausz, R. Kienberger, and N. Karpowicz, “Carrier-envelope-phase-stable, 1.2 mJ, 1.5 cycle laser pulses at 2.1 μm,” Opt. Lett. 37, 4973–4975 (2012).
[Crossref] [PubMed]

C. Manzoni, S.-W. Huang, G. Cirmi, P. Farinello, J. Moses, F. X. Kärtner, and G. Cerullo, “Coherent synthesis of ultra-broadband optical parametric amplifiers,” Opt. Lett. 37, 1880–1882 (2012).
[Crossref] [PubMed]

2011 (4)

G. Sansone, L. Poletto, and M. Nisoli, “High-energy attosecond light sources,” Nat. Photonics 5, 655–663 (2011).
[Crossref]

O. H. Heckl, C. J. Saraceno, C. R. E. Baer, T. Südmeyer, Y. Y. Wang, Y. Cheng, F. Benabid, and U. Keller, “Temporal pulse compression in a xenon-filled Kagome-type hollow-core photonic crystal fiber at high average power,” Opt. Express 19, 19142–19149 (2011).
[Crossref] [PubMed]

A. Wirth, M. T. Hassan, I. Grguras, J. Gagnon, A. Moulet, T. T. Luu, S. Pabst, R. Santra, Z. A. Alahmed, A. M. Azzeer, V. S. Yakovlev, V. Pervak, F. Krausz, and E. Goulielmakis, “Synthesized light transients,” Science 334, 195–200 (2011).
[Crossref] [PubMed]

J. C. Travers, W. Chang, J. Nold, N. Y. Joly, and P. St. J. Russell, “Ultrafast nonlinear optics in gas-filled hollow-core photonic crystal fibers [Invited],” J. Opt. Soc. Am. B 28, A11 (2011).
[Crossref]

2010 (1)

G. Krauss, S. Lohss, T. Hanke, A. Sell, S. Eggert, R. Huber, and A. Leitenstorfer, “Synthesis of a single cycle of light with compact erbium-doped fibre technology,” Nat. Photonics 4, 33–36 (2010).
[Crossref]

2009 (2)

2008 (1)

2007 (1)

2005 (1)

2002 (1)

M. Drescher, M. Hentschel, R. Kienberger, M. Uiberacker, V. Yakovlev, A. Scrinzi, T. Westerwalbesloh, U. Kleineberg, U. Heinzmann, and F. Krausz, “Time-resolved atomic inner-shell spectroscopy,” Nature 419, 803–807 (2002).
[Crossref] [PubMed]

2000 (1)

D. Zhang, Y. Kong, and J.-y. Zhang, “Optical parametric properties of 532-nm-pumped beta-barium-borate near the infrared absorption edge,” Opt. Commun. 184, 485–491 (2000).
[Crossref]

1999 (1)

1997 (2)

1996 (1)

A. Douhal, F. Lahmani, and A. H. Zewail, “Proton-transfer reaction dynamics,” Chem. Phys. 207, 477–498 (1996).
[Crossref]

1992 (1)

A. Dubietis, G. Jonušauskas, and A. Piskarskas, “Powerful femtosecond pulse generation by chirped and stretched pulse parametric amplification in BBO crystal,” Opt. Commun. 88, 437–440 (1992).
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1987 (1)

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Davis, L.

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Graham, E. K.

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Figures (4)

Fig. 1
Fig. 1 Schematic layout of the setup. 1.6 mJ of the output of a 1-ps, Yb:YAG amplifier was used to generate a phase-stable multi-octave supercontinuum directly from the amplifier. At first a small portion of the 1 ps pulses was shortened to 650 fs in a cross-polarized wave generator (XPW) (block 1). Afterwards these pulses were focused into a YAG crystal to generate a supercontinuum (block 2). The rest of the energy containing 1.4 mJ was frequency doubled in a BBO crystal (block 3) and later used to amplify a small portion of the continuum in an optical parametric chirped pulse amplifier (OPCPA) stage (block 4). Later on the amplified pulses were mixed with residual energy of the XPW stage in a BBO crystal for difference frequency generation (block 5). The generated pulses were compressed to 32 fs using several fused silica plates and later on were focused into a YAG crystal for generation of a CEP-stable, multi-octave spectrum. The footprint of the setup is 70×50 cm2. BS: beam splitter; TFP: thin film polarizer; NP: nanoparticle polarizer; F: filter; Si:silicon; FS: fused silica.
Fig. 2
Fig. 2 a) Amplified spectrum in the OPCPA stage. b) The difference frequency generation between the OPCPA and the regenerative amplifier pulses in a 2-mm-thick BBO crystal results in a broadband spectrum centered at 2 μm. The generated pulses are intrinsically CEP-stable. c) The pump spectrum before (blue) and after (red) DFG. While the spectrum of the seed pulses stays unchanged, a hole appears in the pump’s spectrum, as the signature of energy saturation. d) The simulated spectral bandwidth of the generated difference frequency pulses for different seed to pump energy ratio.
Fig. 3
Fig. 3 a) Measured (left) and retrieved (middle) SH-FROG spectrograph and retrieved temporal intensity (right) of the difference frequency pulses. Gerror = 7.8 × 10−3. The pulse is compressed to 32 fs using bulk material. b) Spectrum of the multi-octave continuum containing 4 μJ generated in a 6 mm YAG crystal. Inset: transverse intensity profile of the supercontinuum after a beamsplitter for 670–1700 nm (i) and 1700–2500 nm (ii). c) Spectral bandwidth, obtained energy, and CEP-stability at each stage of the setup. λ0 shows the central wavelength of the generated pulses. XPW: cross-polarized wave generation; SC: supercontinuum; OPCPA: optical parametric chirped pulse amplification; DFG: difference frequency generation.
Fig. 4
Fig. 4 a) Layout of the f-2f interferometer for monitoring the intensity and phase stability of the supercontinuum. The fundamental and its orthogonally polarized second harmonic, produced in a LiNbO3 crystal are interferometrically overlapped by projecting them onto the same polarization state using a beamsplitter cube. b) The resolved fringes in the f-2f interferometer (left) and variation of the f-2f interference pattern over 600 s (right). c) Histogram (left) and reconstructed CEP fluctuations obtained from the f-2f measurement. The retrieved fluctuations yield a 144 mrad CEP jitter over 600 s measurement time (detector’s integration time: 4 ms). d) reconstructed CEP fluctuations over 6000 s yielding 90 mrad jitter (detector’s integration time: 30 ms). BC: beam combiner; BS: beam splitter.

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